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For a convective instability a localized perturbation grows exponentially at some moving frame and decays at fixed point. For an absolute instability the perturbation grows at any fixed point, see, e.g., E. M. Lifshits and L. P. Pitaevskii, Physical Kinetics (Pergamon Press, Oxford, New York, 1981).
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The opposite case describes the scattering of the incoming wave generated far away from the boundary with the wave vector given by an external source (or opposite boundary). In this case the boundary does not select the structure in the bulk [17]
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The opposite case describes the scattering of the incoming wave generated far away from the boundary with the wave vector given by an external source (or opposite boundary). In this case the boundary does not select the structure in the bulk [17].
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